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Sol Tom Rattan

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0% found this document useful (0 votes)
40 views18 pages

Sol Tom Rattan

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Syed Yousufuddin
Copyright
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2019

MPROVEMENT

Mechanical Engineering

Theory of Machines
Answer Key of Objective & Conventional Questions
1 Mechanisms and Machines

© Copyright: Subject matter to MADE EASY Publications, New Delhi. No part of this book may be reproduced or utilised in any form without the written permission.
1. (c) 14. (6)

2. (c) 15. (1)

3. (a) 16. (c)

4. (a) 17. (1)

5. (c) 19. (c)

6. (a) 20. (c)

7. (d) 21. (b)

8. (d) 22. (a)

9. (d) 23. (b)

10. (a) 24. (b)

11. (c) 25. (1)

12. (d) 26. (a)

13. (d) 27. (180)

„„„„

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Rank Improvement Workbook 3

Solution : 28
In this mechanism

95.7°
50 70
b c

B D
a 20 A
70 d
(a)

μ = 95.7°
C

°
77.6
b c

A D
a d

B (c)
μ = 45.6°

60°
b c

B
a

A d D
(d)

μ = 60°
And the input angle, θ = 60°

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Mechanical Engineering •
4 Theory of Machine

Solution : 29
The mechanism has three sub-chains:
(i) ABC, a slider-crank chain
(ii) ABDE, a four-bar chain
(iii) AEFG, a four-bar chain
(DEF is a locked chain as it has only three links.)
• As the length BC is more than the length AB plus the offset of 2 units, AB acts as a crank and can
revolve about A.
• In the chain ABDE,
Length of the longest link = 8, Length of the shortest link = 4, Length of the other links = 8 and 6
Since 8 + 4 < 8 + 6, it belongs to the class-I mechanism. In this case as the shortest link is fixed, it is a
double-crank mechanism and thus EF and AG can revolve fully.
• In the chain AEFG,
Length of the longest link = 8, Length of the shortest link = 4, Length of the other links = 6 and 6
Since 8 + 4 = 6 + 6, it belongs to the class-I mechanism. In this case as the shortest link is fixed, it is a
double-crank mechanism and thus EF and AG can revolve fully.
AS DEF is a locked chain with three links, the link EF revolves with the revolving of ED. With the revolving
of ED, AG also revolves.
Solution : 30
(a) The mechanism has a sliding pair. Therefore, its degree of freedom must be found from Gruebler’s
criterion. Total number of links = 8
7
4
5 1
3 6

2
8
1
1
(At the slider, one sliding pair and two turning pairs)
F = 3(N – 1) – 2P1 – P2
= 3(8 – 1) – 2 × 10 – 0 = 1
Thus, it is a mechanism with a single degree of freedom.
(b) The system has a redundant degree of freedom as the rod of the mechanism can slide without
causing any movement in the rest of the mechanism.
∴ Eeffective degree of freedom = 3(N – 1) – 2P1 – P2 – Fr
= 3 (4 – 1) – 2 × 4 – 0 – 1 = 0
As the effective degree of freedom is zero, it is a locked system.

„„„„

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2 Velocity & Acceleration
Analysis

© Copyright: Subject matter to MADE EASY Publications, New Delhi. No part of this book may be reproduced or utilised in any form without the written permission.
1. (b) 12. (67) (66.5 to 67.5)

2. (0.33) 13. (a)

3. (d) 14. (301.59)

4. (c) 15. (2.74)

5. (b) 16. (a)

6. (d) 17. (3)

7. (0) 18. (1000)

8. (b) 19. (45)

9. (1) 20. (2.69)

10. (b) 21. (8.386)

11. (c) 22. (a)

„„„„

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Mechanical Engineering •
6 Theory of Machine

Solution : 23
vd = gd = 0.56 m/s
ωbq = 5.63 rad/s counter-clockwise
ωba = 6.3 rad/s counter-clockwise
Velocity of rubbing at the crank pin
B = 0.0268 m/s
Solution : 24
v s = 0.276 m/s
vpq = 0.177 m/s
ωrs = 0.279 rad/s clockwise

Solution : 25
vd = 2.28 m/s

Solution : 26
αcd = 33.25 rad/s2
Solution : 27
aA/0 = 3.507 × 103 mm/s2
VB = 2.3 × 4 = 9.2 m/s
aB = 2.6 × 105 m/s2
α= 6666.67 rad/s2
Acceleration of mid point aG = 2800 m/s2
Solution : 28
By measurement VR = vector O1r = 1.61 m/s
ωDO2 = 1.112 rad/s anticlockwise about O2
Solution : 29
Length of crank = 25 cm
V = 4.1887 m/s

„„„„

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3 Cams

© Copyright: Subject matter to MADE EASY Publications, New Delhi. No part of this book may be reproduced or utilised in any form without the written permission.
1. (c) 13. (2.37)

2. (c) 14. (720)

3. (c) 15. (0.628)

4. (a) 16. (1.95)

5. (a) 17. (d)

6. (c) 18. (b)

7. (c) 19. (d)

8. (c) 20. (d)

9. (c) 21. (c)

11. (c) 22. (a)

12. (b) 23. (c)

24. (b)

25. (a)

26. (b)

27. (b)

28. (a)

29. (d)

„„„„

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Mechanical Engineering •
8 Theory of Machine

Solution : 30
vmax = 226.3 mm/s
fmax = 3.413 m/s2
During descent vmax = 216 mm/s
fmax = f = 0
Solution : 31
During descent vmax = 824.7 mm/s
vmax = 549.8 mm/s
fmax = 38862 mm/s2 = 38.882 m/s2
fmax = 17272 mm/s2 or 17.272 m/s2
Solution : 32

30 mm
0
φa δ1 φd
0′ 1′ 2′ (a)
2.52
1 2 3′
Velocity

3
4 4′
120° (m/s)
5
5′ (b) 2.64
30
90°

6 464.6
°

12′ 12
Acceleration

11
11′ 6 211.9
10 9 8 7 6′
10′
9′
8′ 6′ 211.9
7′
2
(m/s )
464.6
Solution : 33

1′ O′
2′
1
3′ 2
3 14 14′
4′ δ2 13 13′
4 φa

5 12
12′
δ1 φd
5′ 6 11
11′
6 10
9
7 8
6′ 10′

9′
6′
7′ 8′

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Rank Improvement Workbook 9

vmax = 360 m/s


fmax = 4320 mm/s2 or 4.32 m/s2

Solution : 34
x = 40 ω2 cos θ
N = 609.9 rpm

Solution : 35
The displacement diagram for the given flat reciprocating follower movement will be as:
6 6′ 6′
5
5′ 7′
4 8′
4′

3
3′ 9′
2′ 10′
2
1′ 11′
12′
1
1 2 3 4 5 6 6 7 8 9 10 11 12
Dwell Dwell
Outstroke Return stroke
(φa) (δ1) (δd) (δ2)

Given: φa = 120°, h(lift) = 20 mm, δ1 = 30°, φd = 120°, δ2 = 90°


Motion is SHM both during outward and inward stroke, minimum radius of cam (rc) = 25 mm.
Construction:
25
1. First draw the displacement diagram now construct the cam
a
profile as follows b
1
2. Draw a circle with radius (rc = 25 mm) c 2
3. Take angles (φa, δ1, φd and δ2) in the counter clockwise 3

90

°
d

12
direction if the cam rotation is assumed clockwise 4

4. Divide φa and φd into same number of parts as in the 5


displacement diagram. (Example take 6 equal parts) e
30
6 0° 12 l
12 °
5. Draw radial lines (0-1, 0-2, 0-3,, etc. ....) 11
f 7
6. On the radial lines produced, take distances equal to the 8 10 k
9
lift of the follower beyond the circumference of the circle
with radius rc, i.e., 1 - 1′, 2 - 2′, 3 - 3′, etc. g
j
7. Draw the follower in all the positions by drawing i
perpendiculars to the radial lines at 1′, 2′, 3′, etc. In all the h

positions, the axis of the follower passes through centre O


8. Draw a curve tangential to the flat faces of the follower representing the cam profile.

Solution : 36
Radial component of cam force is given by;
Fr = 61 N
Torque = 0.651 N.m
Solution : 37
In this motion:
(V0)max = 1.2 m/s
a = 72 m/s2

„„„„

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4 Gear and Gear Train

20. (a)

© Copyright: Subject matter to MADE EASY Publications, New Delhi. No part of this book may be reproduced or utilised in any form without the written permission.
21. (a)
1. (c)
22. (c)
2. (7.48)
23. (0.86)
3. (91)
24. (10.29)
4. (360)
25. (9.04)
5. (a)
26. (c)
6. (c)
27. (b)
7. (b)
28. (a)
8. (d)
29. (c)
9. (d)
30. (b)
10. (d)
31. (c)
11. (c)
32. (b)
12. (39207.076)
33. (b)

34. (a)

35. (d)
13. (c)
36. (c)
14. (c)
37. (d)
15. (b)
38. (70)
16. (a)
39. (d)
17. (b)
40. (18)
18. (b)
41. (c)
19. (b) „„„„

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Rank Improvement Workbook 11

Solution : 42
Velocity of sliding = 57049 mm/min = 950.8 mm/s
Maximum velocity of sliding = 1017.1 mm/s
Solution : 43
Addendum of the wheel = 8.3 mm

ra2 = 30271
Addendum of the pinion = 14 mm
Arc of contact = 58.2 mm
Solution : 44
Length of arc of contact = 30.788 mm
n = 1.6334
Angle of action by the pinion, θp = 0.54 radian
θp = 30.95°
(a) = 0.388
(b) = 0.348
(c) = 0
Solution : 45
T = 49.44
n = 1.78
Solution : 46
Addendum, a = 0.8010 m
Stubbing required = 19.9% or 20%
Solution : 47
TF = 72
TS = 18
Speed of P, NP = – 166.67 rpm
Therefore, speed of planet Gear P is 166.67 rpm in opposite direction to S and A.

Solution : 48
Speed of output shaft = – 50 rpm (clockwise)
Speed of output shaft = 39.5 rpm (clockwise)

„„„„

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5 Flywheel and Governors

© Copyright: Subject matter to MADE EASY Publications, New Delhi. No part of this book may be reproduced or utilised in any form without the written permission.
1. (c) 18. (d)

2. (d) 19. (323.6)

3. (d) 20. (991.735)

4. (d) 21. (183.33)

5. (243.17) 22. (22360)

6. (0.04) 23. (0.38)

7. (0.38) 24. (d)

8. (d) 25. (b)

9. (a) 26. (0.51)

10. (d) 27. (31.98)

11 (206.04) 28. (0.0444)

12. (b) 29. (51.3)

13. (a) 30. (31.4)(30 to 33)

14. (a) 31. (b)

15. (c) 32. (c)

16. (d) 33. (c)

17. (a) 34. (c)

35. (a)

36. (d)

„„„„

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Rank Improvement Workbook 13

Solution : 37
m = 1217.4 kg
Solution : 38
I = 293.3 kg.m2

Solution : 39
Power of motor = 4276.5 Watt = 4.28 kW
Solution : 40
Motor power = 0.3 kW
M = 988.68 kg
Solution : 41
N = 167 rpm
Range of speed = 4.163 rpm
Solution : 42
m = 5.2 kg
s = 32.72 N/mm
compression of the spring = 33.2 mm
Solution : 43
I = 1394.58 kg-m2
Solution : 44
K = 0.678%
Solution : 45
N = 430.43 rpm
Solution : 46
Power of engine = 261.8 kW
I = 785.166 kg-m2
α = 2.547 rad/sec2
Solution : 47
Initial compression,S1 = 10.03 cm
x1 = 11.65 cm

„„„„

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Balancing and Gyroscope

© Copyright
„„„„
(d)

(a)

(a)

(a)

(a)

(a)
(c)
10.

11.

12.

13.

14.

15.

16.
© Copyright: Subject matter to MADE EASY Publications, New Delhi. No part of this book may be reproduced or utilised in any form without the written permission.

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6
(d)

(b)

(d)

(b)
(a)

(a)

(a)
(c)

(c)
1.

2.

3.

4.

5.

6.

7.

8.

9.
Rank Improvement Workbook 15

Solution : 17
v = 151 km/h

Solution : 18
mc1 = 3.13 kg at 253°
mc1 = 3.14 kg
Solution : 19
ma = 17.37 kg
θa = 294.6° or 294°36′
ld = –309 mm
lb = – 376 mm
lc = –126 mm

Solution : 20
m4 = 178.7 kg
θ4 = 248.2°
m1 = 178.7 kg = m4
θ1 = 201.8°
Swaying couple = 3030.3 N.m
Variation in tractive force = 10100 N
Balance mass for reciprocating parts only = 74.46 kg
Maximum pressure on rails = 45326 N
Minimum pressure on rails = 23344 N
Velocity of wheels = 88.36 km/h
Solution : 21
m3 = 448 kg
m2 = 438 kg
Solution : 22
R1 = 4431.8 N
R2 = 8223.8 N
R3 = 2567.2 N
R4 = 6359.2 N
R1 = 8158.2 N
R2 = 4366.2 N
R3 = 6426.8 N
R4 = 2632.8 N

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Mechanical Engineering •
16 Theory of Machine

Solution : 23
Reaction at bearing, B = 98.6 N
Reaction at bearing, A = 59.4 N
Solution : 24
mA = 9.67 kg, mD = 7.89 kg
Angular position of the mass at D = 252.7° (w.r.t. B)

Solution : 25
m = 92.8 kg
θ = 201.48°
Solution : 26
Resultant = 8224.6 N
M = 40 kg

„„„„

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7 Vibrations

© Copyright: Subject matter to MADE EASY Publications, New Delhi. No part of this book may be reproduced or utilised in any form without the written permission.
1. (d) 13. (b)

2. (d) 14. (a)

3. (d) 15. (1.11)

4. (a) 16. (c)

5. (a) 17. (b)

6. (3) 18. (2.28)

7. (b) 19. (0.56)

8. (d) 20. (26.74)

9. (d) 21. (1.9052)

10. (d) 22. (a)

11. (b) 23. (0.667)

12.. (a) 24. (1)

25. (8)

26. (2)

27. (0.05)

„„„„

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Mechanical Engineering •
18 Theory of Machine

Solution : 28
1
 + aρg × 2 xx = 0
alρ× 2 xx
2
2g
x + x =0
l
Solution : 29
A = 0.00298 m = 2.98 mm
Solution : 30
fn = 2.85 Hz
Solution : 31
δ= 0.693
C= 45.809 Nm/rad
periodic time of oscillation = 1.503 × 10–3 sec
fn = 669.2 Hz
Solution : 32
2
k1l12 + mgl ⎛ Cl2 ⎞
ωd = −⎜
ml 2 ⎝ 2ml 2 ⎟⎠
Solution : 33
Nc = 2598 r.p.m
Solution : 34
C = 400.824 N/m/s
fd
= 0.99
fn
Td = 0.32 sec
Solution : 35
δ = 0.405
Damping coefficient, C = 32.745 N.m.s/rad
ωd = 4233.72 rad/s
Td = 1.484 × 10–3 s
Solution : 36
FT = 38.6 N
FT = 367 N
Amplitude of the forced vibration of the machine at resonance = 8.7 mm
Solution : 37
C = 2970 N-m/rad
Solution : 38
A = 130 mm
φ = 42.4897°
Solution : 39
k = 1.607 N/mm

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